Abstract:The purpose of manipulating isolated single-wall carbon nanotubes (SWNTs), rather than bundles, has led to an active research in the field of the functionalisation of such carbon compounds. Different ways exist today to obtain some new soluble macromolecules from SWNTs. Here we focus on the fluorination functionalisation. As the solubility properties depend essentially on the functionalisation degree, it is important to develop reliable and simple methods to quantify this degree. The C n F stoichiometry of thr… Show more
“…Figure 7 shows the high resolution scan of the C1s region on a sample of grown SWCNTs from 10 min of growth at 650 C. The spectrum has been fitted with three components; one at 284.4 eV attributed to sp 2 hybridized carbon, a second peak at 285.2 attributed to sp 3 carbon mainly from adventitious carbon from atmospheric contaminants, 13 and finally a peak at 286.8 eV encompassing oxides of carbon such as carboxyl and carbonyl moieties. 31 The XPS data shows predominantly graphitic carbon is present on the surface, in agreement with the Raman data presented earlier. There is a small amount amorphous or sp 3 hybridized carbon present on the surface, possibly from carbonaceous impurities or possibly defect sites along the CNT walls and end groups.…”
In this work a simple and up-scalable technique for creating arrays of high purity carbon nanotubes via plasma enhanced chemical vapor deposition is demonstrated. Inductively coupled plasma enhanced chemical vapor deposition was used with methane and argon mixtures to grow arrays in a repeatable and controllable way. Changing the growth conditions such as temperature and growth time led to a transition between single and multi-walled carbon nanotubes and was investigated. This transition from single to multi-walled carbon nanotubes is attributed to a decrease in catalytic activity with time due to amorphous carbon deposition combined with a higher susceptibility of single-walled nanotubes to plasma etching. Patterning of these arrays was achieved by physical masking during the iron catalyst deposition process. The low growth pressure of 100 mTorr and lack of reducing gas such as ammonia or hydrogen or alumina supporting layer further show this to be a simple yet versatile procedure. These arrays were then characterized using scanning electron microscopy, Raman spectroscopy and x-ray photoelectron spectroscopy. It was also observed that at high temperature (550 °C) single-walled nanotube growth was preferential while lower temperatures (450 °C) produced mainly multi-walled arrays.
“…Figure 7 shows the high resolution scan of the C1s region on a sample of grown SWCNTs from 10 min of growth at 650 C. The spectrum has been fitted with three components; one at 284.4 eV attributed to sp 2 hybridized carbon, a second peak at 285.2 attributed to sp 3 carbon mainly from adventitious carbon from atmospheric contaminants, 13 and finally a peak at 286.8 eV encompassing oxides of carbon such as carboxyl and carbonyl moieties. 31 The XPS data shows predominantly graphitic carbon is present on the surface, in agreement with the Raman data presented earlier. There is a small amount amorphous or sp 3 hybridized carbon present on the surface, possibly from carbonaceous impurities or possibly defect sites along the CNT walls and end groups.…”
In this work a simple and up-scalable technique for creating arrays of high purity carbon nanotubes via plasma enhanced chemical vapor deposition is demonstrated. Inductively coupled plasma enhanced chemical vapor deposition was used with methane and argon mixtures to grow arrays in a repeatable and controllable way. Changing the growth conditions such as temperature and growth time led to a transition between single and multi-walled carbon nanotubes and was investigated. This transition from single to multi-walled carbon nanotubes is attributed to a decrease in catalytic activity with time due to amorphous carbon deposition combined with a higher susceptibility of single-walled nanotubes to plasma etching. Patterning of these arrays was achieved by physical masking during the iron catalyst deposition process. The low growth pressure of 100 mTorr and lack of reducing gas such as ammonia or hydrogen or alumina supporting layer further show this to be a simple yet versatile procedure. These arrays were then characterized using scanning electron microscopy, Raman spectroscopy and x-ray photoelectron spectroscopy. It was also observed that at high temperature (550 °C) single-walled nanotube growth was preferential while lower temperatures (450 °C) produced mainly multi-walled arrays.
“…There are various ways to fluorinate CNTs, including gas phase routes using atomic fluorine [5], F 2 gas [11], BF 3 vapor [12], and CF 4 plasma functionalization [13]. Fluorine coverage of single walled CNTs increases with increasing temperature, reaching a maximum coverage of C 2 F between 250 and 300 C [14,15].…”
Calculations of fluorine binding and migration on carbon nanotube surfaces show that fluorine forms varying surface superlattices at increasing temperatures. The ordering transition is controlled by the surface migration barrier for fluorine atoms to pass through next neighbor sites on the nanotube, explaining the transition from semi-ionic low coverage to covalent high coverage fluorination observed experimentally for gas phase fluorination between 200 and 250 C. The effect of solvents on fluorine binding and surface diffusion is explored.
“…The other important point that is worth noting is that, when one does Raman scattering experiments, the resonance is very sharp and therefore, it is somewhat difficult and even speculative to try to determine precisely any diameter distribution in a given sample. It remains that when Raman scattering is performed in the red range excitations, some attempts have been made to assign RBM bands to isolated tubes on one hand and bundles tubes on the other hand [10], even if one knows that they can be different in terms of diameters. Another important point is related to non-linear effects, more precisely stimulated Raman scattering effects.…”
Section: Use Of Non-linear Effects To Recognize Nanotubes In Bundlesmentioning
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